PeterDonis
Mentor
- 49,389
- 25,426
nitsuj said:How is c governed by the fine structure constant in the sense of; If it's "stronger" then is c faster?
On our current understanding, dimensionless constants like the fine structure constant are actually the more "fundamental" quantities; dimensionful quantities like ##c## are actually artifacts of our system of units (after all, we can always choose units to make ##c = 1##). So it's not so much that increasing the fine structure constant makes the speed of light "faster", as that increasing the fine structure constant, which increases the strength of the electromagnetic interaction, changes the behavior of the things we use to measure how "fast" light travels.
In the case of johne618's proposed experiment (which I'll modify slightly to eliminate any issues with measuring time intervals at spatially separated locations), if we emit a beam of laser light that reflects off a mirror a distance ##L## away and comes back and is detected, and we count the number of atomic clock oscillations between the emission and detection of the beam, if ##\alpha## changes, that changes both the interaction strength that governs the atomic clock oscillations, *and* the interaction strength that governs the measuring tools we used to measure the distance ##L##.
Heuristically, increasing ##\alpha## makes the atomic clock oscillations "faster" (electrons are pulled towards the nucleus more strongly, so they have to orbit faster to maintain a stable orbit), and it "shortens" the measuring tools (by strengthening the interactions that hold them together) that are used to determine ##L##, and the two effects should cancel each other out, at least to a first approximation, which is why I said I didn't think this experiment would work anyway, because I don't think it would give different results even if the fine structure constant *did* change. (But, as I said, there are other ways to estimate what the fine structure constant was in the past.)